2015
DOI: 10.1021/acs.jpcc.5b00047
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Biphasic Resistive Pulses and Ion Concentration Modulation during Particle Translocation through Cylindrical Nanopores

Abstract: We investigated the biphasic resistive pulses during particle translocation through cylindrical nanopores at low salt concentration by simulation, and the effects of electrolyte concentration, surface charge, electric potential, and pore geometry were systematically discussed. The formation of positive peaks in the pulses is ascribed to the surface charge on the particle and the pore. The peak current enhancement/decline ratio increases linearly with the particle surface charge density but decreases with the s… Show more

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Cited by 22 publications
(26 citation statements)
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“…The surface charge density of SiN x nanopore was set as −0.005 C m −2 at pH 8 and 0.005 C m −2 at pH 2. [29,56] ICR phenomenon could be observed in both acidic and alkaline simulation. In pH 2, absolute magnitude of current at positive voltage was less than that at negative voltage, which was consistent with the experimental result.…”
Section: (6 Of 8)mentioning
confidence: 85%
“…The surface charge density of SiN x nanopore was set as −0.005 C m −2 at pH 8 and 0.005 C m −2 at pH 2. [29,56] ICR phenomenon could be observed in both acidic and alkaline simulation. In pH 2, absolute magnitude of current at positive voltage was less than that at negative voltage, which was consistent with the experimental result.…”
Section: (6 Of 8)mentioning
confidence: 85%
“…Similarly,b yt heoretically analyzing the bubble-substrate interactions in 1mm NaCl of pH 3.0, 8.0 and 10.0 (Figure 4), the corresponding Y OTS values were determineda nd listed in Ta ble 1, showing that OTS-mica surfaceb ecomes more negatively charged with increasing solution pH. [22] It is noticeable that ad istinct jump-in behaviorw as observed in the interaction force curve for the case of 1mm NaCl of pH % 3.0, indicating that the bubble attached onto the hydrophobic substrate duringt he approachingp rocess. This bubble attachment phenomenono nto OTS-mica could arise from the fact that the weak EDL repulsion in this case was not able to resist the strongH Ba ttraction (with ad ecay length of D 0 % 1.0 nm here), which was different from the case of bubble-bubble interaction under the same condition where the EDL repulsion (Y Bub = À23 AE 3mV) was stronge nough to overcome the HB attraction between two air bubbles (with ad ecay length D 0 of % 0.3 nm) [15a, 16h, 17c] and thus stabilize the confined thin water film.…”
Section: Resultsmentioning
confidence: 99%
“…[158][159][160] The increase in electric current is at least partially mediated by increased concentration of positive counterions, which are attracted by the negatively charged DNA into the pore. 161,162 Nevertheless, the microscopic origins of this non-intuitive phenomenon are not yet completely understood.…”
Section: Physics Of Confined Dna: From the Odijk To The De Gennes Regimementioning
confidence: 99%